35 research outputs found

    Dynamical scaling in branching models for seismicity

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    We propose a branching process based on a dynamical scaling hypothesis relating time and mass. In the context of earthquake occurrence, we show that experimental power laws in size and time distribution naturally originate solely from this scaling hypothesis. We present a numerical protocol able to generate a synthetic catalog with an arbitrary large number of events. The numerical data reproduce the hierarchical organization in time and magnitude of experimental inter-event time distribution.Comment: 3 figures to appear on Physical Review Letter

    Evaluating the incompleteness magnitude using an unbiased estimate of the bb value

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    The evaluation of the bb value of the Gutenberg-Richter (GR) law, for a sample composed of nn earthquakes, presents a systematic positive bias δb\delta b which is proportional to 1/n1/n, as already observed by Ogata \& Yamashina (1986). In this study we show how to incorporate in δb\delta b the bias introduced by deviations from the GR law. More precisely we show that δb\delta b is proportional to the square of the variability coefficient CVCV, defined as the ratio between {the standard deviation of the magnitude distribution and its mean value.} When the magnitude distribution follows the GR law CV=1CV=1 and this allows us to introduce a new procedure, based on the dependence of bb on nn, which allows us to {identify} the incompleteness magnitude mcm_c as the threshold magnitude leading to CV=1CV=1. The method is tested on synthetic catalogs and it is applied to estimate mcm_c in Southern California, Japan and New Zealand

    Subduction age and stress state control on seismicity in the NW Pacific subducting plate

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    Intermediate depth (70-300 km) and deep (> 300 km) earthquakes have always been puzzling Earth scientists: their occurrence is a paradox, since the ductile behavior of rocks and the high confining pressure with increasing depths would theoretically preclude brittle failure and frictional sliding. The mechanisms proposed to explain deep earthquakes, mainly depending on the subducting plate age and stress state, are generally expressed by single parameters, unsuitable to comprehensively account for differences among distinct subduction zones or within the same slab. We analyze the Kurile and Izu-Bonin intraslab seismicity and detail the Gutenberg-Richter b-value along the subducted planes, interpreting its variation in terms of stress state, analogously to what usually done for shallow earthquakes. We demonstrate that, despite the slabs different properties (e.g., lithospheric age, stress state, dehydration rate), in both cases deep earthquakes are restricted to depths characterized by equal age from subduction initiation and are driven by stress regimes affected by the persistence of the metastable olivine wedge

    Unjamming dynamics: the micromechanics of a seismic fault model

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    The unjamming transition of granular systems is investigated in a seismic fault model via three dimensional Molecular Dynamics simulations. A two--time force--force correlation function, and a susceptibility related to the system response to pressure changes, allow to characterize the stick--slip dynamics, consisting in large slips and microslips leading to creep motion. The correlation function unveils the micromechanical changes occurring both during microslips and slips. The susceptibility encodes the magnitude of the incoming microslip.Comment: See http://prl.aps.org/supplemental/PRL/v104/i23/e238001 for related animation

    How long is an aftershock sequence?

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    The occurrence of a mainschok is always followed by aftershocks spatially distributed within the fault area. The aftershocks rate decay with time is described by the empirical Omori law which was inferred by catalogues analysis. The sequences discrimination within catalogues is not a straightforward operation, especially for low-magnitude mainshocks. Here, we describe the rate decay of the Omori law obtained using different sequence discrimination tools and we discover that, when the background seismicity is excluded, the sequences tend to last for the temporal extension of the catalogue

    How Long is an Aftershock Sequence?

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